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Upscaling and Inverse Modeling of Groundwater Flow and Mass ...

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10 CHAPTER 2. A COMPARATIVE STUDY OF THREE- . . .<br />

Table 2.1: Variogram parameters for the model fit in Figure 2.2<br />

Model Type Sill Range [m]<br />

c ax ay az<br />

Nugget 0.424<br />

Spherical 3.820 32 80 4.1<br />

Hole effect 0.891 ∞ 80 ∞<br />

where h = (hx, hy, hz) is the separation vector, ax1 , ay1 , az1 are the ranges<br />

<strong>of</strong> the spherical variogram, ax2 , ay2 , az2 are the ranges <strong>of</strong> the hole-effect variogram,<br />

∥ · ∥ denotes vector modulus, c0 is the nugget, c1 is the sill <strong>of</strong> the<br />

spherical model, c2 is the sill <strong>of</strong> the hole-effect model, with the y-axis oriented<br />

parallel to the flow direction, the x-axis is orthogonal to it on the horizontal<br />

plane, <strong>and</strong> the z-axis is parallel to the vertical direction. The parameter values<br />

used to fit the experimental variogram are given in Table 2.1. Notice that ay2 ,<br />

<strong>and</strong> az2 are equal to infinity, meaning that the hole-effect is only present along<br />

the flow direction. The fitted model is also shown in Figure 2.2.<br />

Figure 2.2: Horizontal <strong>and</strong> vertical experimental variograms, <strong>and</strong> fitted model,<br />

for the lnK flowmeter data. The rotation angle <strong>of</strong> the directional variograms<br />

is measured in degrees clockwise from the positive y-axis.

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